Transient regime in second harmonic generation

被引:1
|
作者
Szeftel, Jacob [1 ]
Sandeau, Laure [2 ]
Sandeau, Nicolas [3 ]
Delezoide, Camille [1 ]
Khater, Antoine [4 ]
机构
[1] ENS Cachan, LPQM, F-94230 Cachan, France
[2] PixInBio SAS, CMP, F-13541 Gardanne, France
[3] Aix Marseille Univ, CNRS, Ecole Cent Marseille, Inst Fresnel, F-13013 Marseille, France
[4] Univ Maine, Lab PEC, UMR 6087, F-72000 Le Mans, France
关键词
Nonlinear optics; Harmonic generation; Frequency conversion;
D O I
10.1016/j.optcom.2013.04.053
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
The time growth of the electromagnetic field at the fundamental and double frequencies is studied from the very onset of the second harmonic generation (SHG) process for a set of dipoles lacking a symmetry centre and exhibiting a nonresonant coupling with a classical electromagnetic field. This approach consists first of solving the Schrodinger equation by applying a generalised Rabi rotation to the Hamiltonian describing the light-dipole interaction. This rotation has been devised for the resulting Hamiltonian to show up time-independent for both components of the electromagnetic field at the fundamental frequency and the second harmonic one. Then an energy conservation argument, derived from the Poynting theorem, is introduced to work out an additional relationship between the electromagnetic field and its associated electric polarisation. Finally this analysis yields the full time behaviour of all physical quantities of interest. The calculated results reproduce accurately both the observed spatial oscillations of the SHG intensity (Maker's fringes) and its power law dependence on the intensity of the incoming light at the fundamental frequency. (C) 2013 Elsevier B.V. All rights reserved.
引用
收藏
页码:107 / 112
页数:6
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